Wave Scattering by Small Bodies of Arbitrary Shapes

Various definitions of optimality of numerical methods and a detailed bibliography can be found in [7], [154]. Let us recall the definitions of algorithms, optimal with respect to accuracy, for calculating weakly singular integrals.
Consider the quadrature formula:
| (A.3) | |
where coefficients
and nodes
are arbitrary. Here
.
The error of quadrature formula (A.3) is defined as
The error of quadrature formula (A.3) on the class ? is defined as
Define the functional
The quadrature rformula with the coefficients
and the nodes
is optimal, asymptotically optimal, optimal with respect to order on the class ? among all quadrature rules of type (A.3) provided that:
The symbol ? ? ? means A ? ? ? ? B ?, where 0 < A, B < ?.
Consider the quadrature rule
| (A.4) | |
where coefficients p k( t 1, t 2) and nodes ( M k) are arbitrary.
The error of quadrature formula (A.4) is defined as
The error of quadrature rule (A.4) on the class ? is defined as
Define the functional
The quadrature rule with the coefficients
and the nodes
is optimal, asymptotically optimal, optimal with respect to order on the class ? among all quadrature rules of the type (A.4) provided that:
| (A.5) | |
By
the error of optimal cubature formulas on the class ? is defined. One has
.